stat mech Flashcards

1
Q

zeroth law

A

if A and B are in equilibrium and B is in equilbrium with c then A and C are in equilibrium

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2
Q

first law

A

work is a state function - the work required to go between states is independent of path

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3
Q

adiabatic expansion

A

no heat - pressure and volume change, temp doesn’t

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4
Q

heat capacity

A

partial of heat with respect to Temp at constant V or P

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5
Q

Ideal gas law using heat capacities

A

Cp-Cv = PV/T = Nkb

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6
Q

second law

A

there cannot be complete conversion of heat to work

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7
Q

draw a pv diagram

A

adiabatic and isotherm curve

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8
Q

adiabatic curve solution

A

PV^gamma for gamm=5/3

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9
Q

entropy equation

A
dQ = TdS
S= kb ln(omega)
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10
Q

what equaitno is implied by the first law

A

dE = dQ+dW

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11
Q

enthalpy

A

cp = dH/dT``

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12
Q

Helmholtz free energy

A

F = E-TS

–isothermal transformations with no work

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13
Q

Gibbs free energy

A

–isothermal transformation with constant external work

G = E-TS-W

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14
Q

extensive, fundamental thermo equation

A

dE = TdS+Fdx+mudN

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15
Q

maxwell relations

A

these follow from the commutative rule of derivatives and give relations between the partial derivates at a constant variable to another (based on fund..eq)

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16
Q

How to find stable points

A

minimum of U or minimum of enthalpy (H= U-Fx) if there is an external force

17
Q

Third law

A

The entropy of all systems at absolute zero can be taken as the universal constant= zero

18
Q

Liouvilles theorem

A

phase space density behave like an incompressible fluid, {A,B} = -{B,A}

19
Q

microcanonical ensemble

A

mechanically and adiabatically isolated
macrostate M=(E,x)

omega = int(dE1*exp(S1(E1)-S2(E-E1)/kb)

20
Q

two-level system

A

H = eN, where N is number of excited impurities

Omega = N!/N1!/(N-N1)!

1/T = dS/dE at constant N , then solve for E

21
Q

energy of an ideal gas with f degrees of freedom

A

E = (f/2)*(NkT)

22
Q

canonical ensemble

A
temperature of the system is known 
- it has a resevoir from which to draw heat 
- no external work
- uses the partition function 
Z =sum_u exp(-BH(u))
23
Q

Gibbs canonical ensemble

A

Heat and work are allowed
no chemical work
Z = sum_(u,x) exp(BJ.x-BH(u))
G = -kbTln(Z)

24
Q

grand canonical ensemble

A

chemical work and heat
no mechanical work
Z = sum_(u) exp(BuN(u)-BH(u))

25
Q

Which two ensembles are identical in the thermodynamic limit

A

canonical and microcanonical

26
Q

explain phase transitions

A

exist only in the thermodynamic limit (N=>infinity)
critical points = correspond to singularities in free energy
first order are discontinuous - lines separating phases
second order are continous - like past the critical point for ice

27
Q

monte carlo simulations

A

better explanation

28
Q

brownian motion

A

188 in kardar field